化工进展 ›› 2019, Vol. 38 ›› Issue (9): 4164-4173.DOI: 10.16085/j.issn.1000-6613.2018-2398

• 材料科学与技术 • 上一篇    下一篇

氧化石墨烯表面的饱和池沸腾强化传热实验

毛兰1,2(),周文斌1(),胡学功1,2(),何雨1,2,张桂英1,单龙1   

  1. 1. 中国科学院工程热物理研究所,北京 100190
    2. 中国科学院大学,北京 100049
  • 收稿日期:2018-12-11 出版日期:2019-09-05 发布日期:2019-09-05
  • 通讯作者: 周文斌,胡学功
  • 作者简介:毛兰(1993—),女,博士研究生,研究方向为微纳尺度传热学。E-mail:maolan@iet.cn
  • 基金资助:
    国家重点研发计划(2017YFB0403200)

Enhanced pool boiling heat transfer performance on graphene oxide nanocoating surface

Lan MAO1,2(),Wenbin ZHOU1(),Xuegong HU1,2(),Yu HE1,2,Guiying ZHANG1,Long SHAN1   

  1. 1. Institute of Engineering Thermophysics, Chinese Academy of Sciences, Beijing 100190, China
    2. University of Chinese Academy of Sciences, Beijing 100049, China
  • Received:2018-12-11 Online:2019-09-05 Published:2019-09-05
  • Contact: Wenbin ZHOU,Xuegong HU

摘要:

利用氧化石墨烯(GO)纳米片沸腾自组装法(self-assembly)制备出GO纳米表面,以蒸馏水为液体工质,对常压下GO纳米表面和光滑铜平面的饱和池沸腾换热特性进行了对比实验研究,并用高速摄像机拍摄了汽泡的动态行为。结果表明,GO纳米表面降低了换热壁面的过热度,其临界热流密度(CHF)和换热系数(HTC)分别达到了208W/cm2和7.25W/(cm2?K),较光滑铜平面分别提高了66.4%和86.9%。分析认为,是铜基底表面沉积的润湿性优异的高导热二维GO层状结构促使了CHF提高。汽泡可视化观察发现,相比于光滑铜平面,较低热流密度时,相同热流下GO纳米表面上汽泡脱离直径较小,脱离频率较高,汽化核心增多;较高热流密度时,光滑铜平面汽泡合并现象更严重,即GO纳米表面能延缓导致CHF产生的表面蒸汽膜的出现。

关键词: 纳米结构, 池沸腾, 汽泡, 相变, 可视化, 传热

Abstract:

The use of nanostructured surfaces to improve the pool boiling heat transfer has been recognized as an effective method. Graphene oxide (GO) nanocoating surface was fabricated by GO nanosheets self-assembly under nucleate pool boiling conditions in present study. And the saturated pool boiling heat transfer on the GO nanocoating surface and copper plain surface were experimentally investigated under atmospheric pressure and with distilled water as working fluid. A high-speed camera was used to visualize the bubble dynamic growth process, and the bubble departure diameter and frequencies at different heat fluxes were obtained. The results showed that the superheat of GO nanocoating surface was lower than that of the copper plain surface at the same heat flux. The critical heat flux (CHF) and heat transfer coefficient (HTC) of GO nanocoating surface reached 208W/cm2 and 7.25W/(cm2·K) respectively, which increased by 66.4% and 86.9% compared to those of the copper plain surface. The enhanced heat transfer performance was attributed to the favorable wettability and superior thermal conductivity of deposited two-dimensional GO layers on the copper substrate. Additionally, visualizations at low heat flux showed that when compared to copper plain surface, the bubble departure diameter of GO nanocoating surface was smaller and the frequencies were higher and the nucleus sites were more. The GO nanocoating surface was more conducive to bubble growth and departure. And at high heat flux, the bubble coalescence on the copper plain surface was more severe than that on the GO nanocoating surface. That is, the GO nanocoating surface can delay the appearance of the vapor blanket over the heating surface which triggers the CHF.

Key words: nanostructure, pool boiling, bubble, phase change, visualization, heat transfer

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